From: CellExcite: an efficient simulation environment for excitable cells
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d
r
3 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeG4mamdaleqaaOGaemOCaihaaa@344B@
2r
7 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeG4naCdaleqaaOGaemOCaihaaa@3453@
3r
2 3 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobjugCbiabikdaYOWaaOaaaeaajugCbiabiodaZaWcbeaakiabdkhaYbaa@3626@
13 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeGymaeJaeG4mamdaleqaaOGaemOCaihaaa@353B@
4r
ν r Δ ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUPWaaSbaaSqaaiabdkhaYbqabaaabeqaaKqzWfGaeyiLdqeaaOWaaeWaaeaacqWGKbazaiaawIcacaGLPaaaaaa@39A1@
−6
N/A
ν Δ 2 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUbWcbeqaaKqzWfGaeyiLdqeaaOWaaSbaaSqaaiabikdaYiabdkhaYbqabaGcdaqadaqaaiabdsgaKbGaayjkaiaawMcaaaaa@3A9E@
−42.96
4.48
1.68
ν Δ 3 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaqcfa4aaCbiaOqaaKqzafGaeqyVd4galeqabaqcLbuacqGHuoaraaqcfa4aaSbaaeaacqaIZaWmcqWGYbGCaeqaaiaaykW7daqadaqaaiabdsgaKbGaayjkaiaawMcaaaaa@3CD2@
−191.70
14.39
7.38
5.29
1.94
−726.24
42.52
25.79
20.08
9.48
5.75
2.72
2.12